Torsion meter



Feb. 19, 1952 w. H. T. HOLDEN 2,586,540

TORSION METER Filed Feb. 26, 1948 3 Sheets-Sheet 1 INVENTOR WILLIAM HIHOLDEN BY O MMM TORNEY F 19, 1952 w. H. T. HOLDEN 2,586,540

TORSION METER Filed Feb. 26, 1948 3 Sheets-Sheet 2 INVENTOR WILLIAM H.T. HOLDEN TTORNEY Feb. 19, 1952 w. H. T. HOLDEN TORSION METER Filed Feb. 26, 1948 3 Sheets-Sheet 5 I62 ,6] INVENTOR WILLIAM H. T. HOLDEN BY i-HJMM TTORNEY Patented Feb. 19, 1952 UNITED STATES PATENT OFFICE TORSION METER William H. T. Holden, Woodside, N. Y.,.assignor to Bell Telephone Laboratories, Incorporated, New York, N. Y., a corporation of New York Application February 26, 1948, Serial No. 11,209

2 Claims.

This invention relates to apparatus and a method for measuring the torque or the power transmitted by a rotating shaft.

An object of the invention is to'provide an accurate and inexpensive apparatus and method.

for measuring the torque of a rotating shaft. An advantageous feature of the invention is that it may satisfactorily be used in connection with a shaft rotating at almost any speed.

Another object of the present invention isto provide apparatus and a method for producing.

a measurement dependent upon the torsional deflection between longitudinally spaced portions of a rotating shaft. For example-the. present invention is applicable for producing measurements of power transmitted by such a shaft, In one embodiment, the invention provides a. ethod and means for determining both thetorque and the speed of the shaft, and for combining these quantities to produce an indication of power.

The above-mentioned,as well as other objects,

together with the many advantages obtainable by the practice'of the present invention, will be. readily comprehended by persons skilledin the art by reference to the following detailed description taken'in connection with the annexed drawings which respectively describe and illustrate preferred embodiments of the invention; and wherein:

Figs. 1, 2 and 3 representthree difierent embodiments of apparatus for measuring'the torque transmitted by a rotating shaft, featuring the use of light beams and pho'totubes responsive to same. Fig. l is aschematicplan-view, and Figs; 2 and 3 are schematic elevational views, certain portions being shown in section;

Fig, 4 is a cross-sectional view of a portion of the apparatus shown in Fig. 3, looking in a direction parallel to theshaft, the sectional plane being indicated in Fig. 3, at the line 4-4;

Fig. 5 is a circuit-diagram showing an electrical circuit in which thephototubesofFigs. 3 and 4 are connected, for deriving a voltage de-.- termined by the torqueof the shaft, a generator for producing avoltage determined by the speed of the shaft, and means for combining these-voltages in order to obtain a'response determlned by the power transmittedby the shaft;

Fig, 6 is aschematic diagram o f anotherembodiment of apparatus for measuring the torque tand a phasersensitive circuitconnected enerato'rs; and 1 otating shaft, featuringthe use of generae riven by longitudinallyspacedvportions of I Fig. 7 is a schematic diagram of still another embodiment of. apparatus adapted to measure the torque and the power transmitted by a rotating shaft, featuring the use of synchros having rotors driven by longitudinally separated portions of the shaft.

in more detail.

In illustrative embodirnents of the present invention there is provided a first movable element driven in a closed path through a field of energy by a first portion ofthe shaft, a second element driven in a closed path through a field of energy by a second portion of theshaft displaced longitudinally of said shaft from said first portion, the respective motions of said movable elements having a timed relationship or phase .diflerence Embodiment shown inFig, 1 Reference is made -to Fig.- 1. In this figure there i is illustrated apparatus for measuring the torque-- of arotating shaft in terms of its torsional deflection', comprising means for directing a beam of light'parallel to the shaft, a phototube positioned in the path of said beam, rotary slotted disc-like means, such as two gear-like rotors, carried by the shaft, arranged so that in the absence of torsional deflection of the-shaft, the teeth of onegear are aligned with the slots between the'teeth of the other gear, and'so that their-combined effect is to darken the phototube when there is no torsional deflection. When there is torsional deflection in the shaft, a portion ofthe respective slots 7 of one gear coincides with a portion of the slots of the other gear, and the result is that the light beam. is intermittently-allowed to strike the phototube, forintervals'the duration of which is Y determined by. the torsional deflection of the shaft. The phototube is connected-to electrical circuit means including an instrument adapted to produce an indication. determined by the dura-.

tion of the intervals during whichthephototube is. illuminated., This instrument may be cali-.v brated ;163021 torque directly.

The embodiment of Fig, 1 may now be described There is shown a rotating shaft,

10. It may be assumed that it is desired to measure the torque transmitted by this shaft. There is provided a, light source such as a lamp II and optical means including a collimating lens 12 adapted to direct light from said source in a narrow beam parallel to said shaft through a lens 13 toward a light-sensitive device such as a phototube I4 having electrodes including an anode l5 and a cathode Hi. It will be understood that the lamp I I, the lens [2, the lens l3 and the phototube M are stationary, and do not move when the shaft rotates.

The lamp H may be considered to be on continuously during operation of the apparatus. Light from this lamp illuminates the phototube 14, in the absence of any means in the path of the light beam for interrupting same. There is provided means in the path of the light beam for modulating or intermittently interrupting the beam, including movable elements respectively driven by longitudinally separated portions of the shaft. More particularly, as a portion of such means, there is in the present embodiment provided a gear ll of metal or other opaque material, carried by the shaft at a station A. The gear ii is shaped to have teeth 18 adapted to pass through the light beam, for interrupting or modulating same, and slots or openings 19 between said teeth, adapted to allow the light beam to pass through the gear.

In the embodiment shown in Fig. 1 it may conveniently be assumed that when a gear tooth is is directly in the path of the beam, no light may pass to the right of the gear 11. It may like- Wise be assumed that when a slot I9 is directly in the line of the beam, the light passes through the gear I! unimpeded. The invention is not, however, limited to this particular embodiment. Instead of the gear I! acting alternately to interpose perfectly-opaque teeth is and perfectlylight-transmitting slots 19, the gear H might comprise alternate portions which are only relatively opaque and relatively light transmitting, respectively.

Carried by the shaft ill at a station B displaced longitudinally from the station A is a gear I 20 similar to the gear ll, having teeth 2| and slots 22. Supported by a frame is a stationary shield 23, having a slot 23a therein, adjacent the gear 23, adapted to limit the light beam to the desired width, that is, to approximately the width of a gear slot, thereby preventing any tendency for the light to pass through slots of the gear 20 except when they are in the proper position. Means not shown are provided for initially adjusting the alignment of the gear 20 relative to the gear 11 so that in the absence of torsional deflection of the shaft Hi, the slots of the gear I! are aligned with the teeth of the gear 20, and the teeth of the gear 5'! are aligned with the slots of the gear 20. After the gears are thus aligned, they are firmly afiixed to the shaft, so that any torsional deflection of the shaft between the stations A and B will produce a relative angular movement between the gears 11 and 20. It may be seen that if the shaft is rotating with virtually no torsional deflection, no light will reach the phototube l4 since the combined effect of the gears i1 and 23 is to block oif all light from the phototube. If, however, there is appreciable torsional deflection of the shaft between stations A and B, then portions of slots 19 of the gear I! will become aligned with portions of slots 22 of the gear 26, thereby allowing light to reach the phototube when the shaft is in certain angular positions. Moreover, as the torsional deflection increases, the extent to which slots of the respective gears coincide is increased, thereby increasing the duration of the intervals during which the phototube is illuminated.

The shape of an individual gear tooth may be such that the sides of the tooth are parallel to a diameter of the gear passing through the center of the tooth. The result of this arrangement is that the area of the opening provided by the combined effect of the gears is approximately linear with torsional deflection.

The anode I5 of the phototube i4 is connected to a source of positive potential at a terminal 24 and the cathode i6 is connected to a terminal 25a of a load resistor 25, the other terminal of this resistor being connected to ground. As a result of the previously described intermittent illumination of the phototube, current pulses are caused to flow through the phototube and the resistor 25, thereby producing voltage pulses at the terminal 25a, the pulse length being determined by the torsional deflection of the shaft. The terminal 25a is connected through a resistor 25 to the grid 21 of a cathode follower including a vacuum tube 28. The anode 33 is connected to a source of positive potential at a terminal 3i. The cathode 32 is connected through a resistor 33 and an adjustable source 34 of bias potential to ground, the source 34 being arranged to maintain the cathode 32 at a positive potential with respect to the grid 21. In one embodiment, the bias source 34 is arranged to maintain the cathode 32 at a potential sufficiently positive with respect to the grid 21 to bias the tube 28 just to cut-off. The grid 21 is connected through a capacitor 35 to the junction between the resistor 33 and the potential source 34. The resistor 26 and the capacitor 35 may be considered to comprise a low-pass filter. Circuit constants are so chosen that this filter removes or shunts to ground alternating components of a frequency corresponding to the frequency with which gear teeth pass through the light beam, and higher components. Thus upon the appearance of positive voltage pulses at the terminal 25a, the upper plate of the capacitor 35 will become charged positively through the resistor 26. Upon the termination of a pulse at the point 25a, as when the phototube I4 is momentarily cut off because of being darkened, the capacitor 35 will begin to discharge slowly through the resistors 26 and 25. It may be seen that if at the point 25a there appears a series of voltage pulses of constant amplitude, then there will appear at the grid 21 of the oathode follower a potential proportional to or determined by the duration of these pulses and hence by the torsional deflection of the shaft. In other words, the capacitor 35 may be considered to perform, with its associated resistors, an integrating function so as to provide at the grid 21 a potential determined by the time integral over a cycle of the periodic voltage appearing at the point 25a. A similar voltage drop will appear across the cathode resistor 33 of the cathode follower.

The ends of the resistor 33 are connected to output terminals 36 for the system. As shown in Fig. 1, an indicator such as a direct current voltmeter 31 may be connected to the terminals 36 for indicating the voltage appearing across the resistor 33. This voltmeter may be calibrated to read torque directly.

Instead of employing the source 34 to bias the cathode follower to cut-ofh'this source may be shaft.

omitted, and the calibration of the voltmeter or its zero-set may be arranged to take into account the voltage drop which will appear across the resistor 33 for zero torsional deflection.

In certain other uses for the invention, the terminals 36 may be connected to other apparatus in order to derivea measurement dependent upon torque, such as a measurement of the power transmitted by the shaft. In such an embodiment there would be provided means such as a generator for deriving a voltage proportional to the speed of the shaft, and this voltage, together with the voltage from the terminals 36 would be applied to a multiplying device in order to derive an indication of power. Such a multiplying device will be described at a subsequent point.

It may be seen that there is provided a first movable element. such as for example a tooth of the gear I1, driven in a closed path through a field of light energy by a first portion of the shaft, a second movable element, such as a tooth 2| of the gear 29 driven in a closed path through a field of light energy by a second portion of the shaft displaced longitudinally from the first portion, the respective motions of these movable elements having a phase difference determined by the torsional deflection of the shaft between these portions, and there is further provided comparison means including the phototube I4 respone sive to this phase difference adapted to produce an electrical voltage determined thereby, and measuring means, such as the voltmeter 31, controlled by said comparison means.

Embodiment shown in Fig. 2

Reference is made to Fig. 2 which represents a different embodiment of the present invention. There is shown a rotary shaft 38 and means for measuring the torsional deflection'of this shaft. The apparatus of Fig. 2 employs a phototube, a source of a beam of light, and optical means adapted to direct this beam along a path including various reflecting means, toward the phototube. The shaft is provided with longitudinally separatedportions, each comprising a series of light-absorbing and light-reflecting surfaces, arranged circumferentially with respect to the axis of the shaft. Each of these portions is adapted to pass into the path of the light beam, and to absorb the light or transmit same by reflection, depending upon the angular position of the The combined effect of these longitudinally spaced portions is to darken the phototube if there is no torsional deflection of the shaft. If there is torsional deflection, the combined effect is to illuminate the phototube intermittently during intervals the duration of which is proportional to the torsional deflection. The phototube may be connected to electrical circuit means and indicating means of the type described in connection with Fig. 1.

Fig. 2 may now be described in more detail. In this embodiment, the shaft 38 is provided with rotary light interrupting or modulating means, which may comprise sleeve-like members-39 and 40, adjustably fixed to the shaft, or which may comprise portions of the shaft itself provided with surface regions of a type to be described. The member 39 is provided with a plurality of light-reflecting surfaces or facets 4| and a plurality of dark or light-absorbing surfaces 42, alter-- nately spaced in a circumferential arrangement with respect to the axis of the shaft. The member 40 is also provided with a plurality of lightreflecting surfaces 43 and a plurality of light The purpose of this absorbing surfaces 44, in an arrangement gen erally similar to that of the member 39, but hav ing an alignment to be described. The light reflecting surfaces and the light-absorbing surfaces may all in the present illustration be assumed to be flat and may be considered to be of equal breadth so that they intercept equal angles at the axis of the shaft. The angular position of the member 40 on the shaft is initially adjusted so that when there is no torsional deflection in the shaft the angular positions of the light-absorbing surfaces 44 of the member 40 correspond to the angular positions of the light-reflecting surfaces 41 of the member 39, and the angular positions of the light-reflecting surfaces 43 of the member 40 correspond to the angular positions of the light-absorbing surfaces 42 of the member 39.

As a particularly useful variation, instead of employing longitudinally spaced sleeve-like members 39 and 40, having'light-absorbing and light-.- reflecting surfaces, longitudinally spaced portions of the shaft itself may be painted to have alternate black or light-absorbing and white or light-reflecting areas, arranged in the same general manner as the previously described lightabsorbing and light-reflecting surfaces of the members 39 and 40. In such an embodiment it may be assumed that the light-reflecting and light-absorbing surfaces are cylindrical, comprising the surfaces of the shaft 'itself.

There is provided a lamp 45,, collimating lens means 46 and 41, and a phototube 48. Cooperating with the rotary member 39 is a mirror 49, in

, the path of and at an oblique angle to the light from the lamp 45 and the lens 46. The mirror 49 is adapted to reflect'the light beam toward the member 39. There is provided a mirror 50, similarly obliquely oriented to the axis of the-beam from the lamp, and adapted to receive light re-! flected by the light-reflecting surfaces 4|, when they are opposite the mirrors 49 and 50. The light beam is directed by the mirror 50 in a beam parallel to the shaft, and there is provided .a pair of mirrors 5| and 52, positioned adjacent to and cooperatingwith the rotary member 40 in a manner generally similar to the previously described cooperation of the mirrors 49 and 50 with the member 39. There is provided a shield 53 having a slot 53a therein adapted to provide an aperture such that when an area of the member 40 is illuminated, the end boundaries of the illumie nated area will be straight, that is, will lie in planes perpendicular to the axis of the shaft. U arrangement is to improve the linearity of the operation of the apparatus.

In the absence of torsional deflection of the shaft 38, then when the shaft is in such an angular position that the light beam is reflected by one of the light-reflecting surfaces 4|, the beam will be absorbed by one of the lighteabsorbing surfaces 44. When theshaft has rotated through a small angle such that one of the light reflecting surfaces 43' is in position to reflect the beam, the beam will be intercepted by one of the light-absorbing surfaces 42. COIlSfiQllfillts ly, when there is no torsional deflection, the

phototube 48 is dark, at all -angular positions of the shaft.

If, however, there is torsional deflection in the shaft, the aligmnent between the membersfia and 40 will be changed somewhat. It is contemplated that the angular deflection of the shaft between the'members 39 and 40 will be a small ,fractien of; the angle intercepted .at the axis of the shaf by one of the facets of the members 39 or 40. When such a deflection occurs, there is some effective overlapping of the lightreflecting surfaces 4! and 43, and the combined effect is to illuminate the phototube intermittently for intervals having ahdgration proportional to the deflection of the s a The phototube 48 is connected to electrical circuit means 54 which may for example be of the type described in connection with Fig. 1, adapted to produce at a pair of output terminals 55 a voltage proportional to or determined by the duration of the intervals of illumination of the phototube, and hence determined by the torsional deflection of the shaft. The terminals 55 may be connected to a voltmeter adapted to read torque directly.

A variety of surfaces may be employed to perform the light-absorbin function of the surfaces 42 and 44 and the light-reflecting function of the surfaces 4| and 43 Thus the sur faces M and 43 may be mirror-like, comprising mirrors or polished metal, or may be white or light colored. The surfaces 42 and 44 may be painted a dull black or other dark color. As a variation, the surfaces 42 may be adapted to polarize the light beam in one direction and the surfaces 44 may comprise polarizing surfaces oriented in a direction so that polarized light from the surfaces 4 2 will not be reflected by the surfaces 44.

Embodiment shown in Figs. 3, 4 and Reference is made to Fig. 3, which, together with Figs. 4 and 5, represents a still different embodiment of the present invention. There is shown a rotary shaft 58, and it may be assumed that it is desired to measure the power transmitted by the shaft, as well as the torque and speed of the shaft. There is provided a rotary member 59 having light-reflecting surfaces 69 and light-absorbing surfaces Bl. The light-reflecting surfaces may conveniently be narrower than the light-absorbing surfaces. Also carried by the shaft 58 and spaced longitudinally from the member 59 is a similar member 62 having light-reflecting surfaces 63 and light-absorbing surfaces 64. The members 59 and 62 are supplied with separate beams of light. This light may come from a common source, or may, as in the illustrated embodiment, come from two different sources, such as a lamp 64 and lens 65, for the member 59, and a lamp 66 and lens 61, for the member 62. There is provided a lens 68 and a phototube 69, positioned to receive light reflected by the surfaces 60, when the shaft is in certain angular positions. When the shaft is in angular positions such that the light beam from the lamp 64 and the lens 65 strikes a light-absorbing surface GI, virtually no light reaches the phototube 69.

There is also provided a lens I0 and a phototube H adapted to receive light reflected by the light-reflecting surfaces 63, when the shaft is in certain angular positions, and adapted to receive virtually no light when the beam from the lamp 66 strikes light-absorbing surfaces 66.

The members 59 and 62 are so oriented with relation to one another that when there is no torsional deflection, phototubes 69 and H are simu taneously illuminated, and simultaneously darkened. In other words, assuming that the aforementioned phototubes 69 and H, and their associated light sources and lenses, are at the same angular positions, the members 59 and 62 arev lit initially so aligned that when there is no torsional deflection the light-reflecting surfaces 60 lie in the same planes as the light-reflecting surfaces 63 and the light-absorbing surfaces Bl lie in the same planes as the light-absorbing surfaces 64.

As the shaft rotates, if there were no torsional deflection, the phototubes 69 and H would be illuminated for a brief interval and then. darkened for a somewhat longer interval, in synchronism. 0n the other hand, if there is torsional deflection in the shaft, the phototube '69 will .be alternately illuminated and darkened, and the phototube II will be alternately illuminated and darkened, but these actions will not be in synchronism. There will be a time lag or phase difference, between the moment when one tube is first illuminated and the moment when the other tube is first illuminated. The amount of this phase difference will be determined by the angular deflection of the shaft between the longitudinally spaced members 59 and 62.

It may be assumed that there is a torsional deflection of the shaft in such a direction that the phototube II is illuminated slightly before the phototube 69 is illuminated. More particularly, it may be assumed that the direction of rotation, as seen in Fig. 4, is clockwise, and that the shaft is driven by a driving means located to the right of that portion of the shaft which is shown in Fig. 3. If there were no load, and hence no torsional deflection, the phototubes 69 and H would be illuminated and darkened simultaneously. It may be assumed, however. that there is a load to the left of the shaft of Fig. 3, and that, as stated, the phototube H is illuminated shortly before the phototube 69. There is provided a comparison circuit, illustrated in Fig. 5, adapted to be sensitive to the phase difference or time relationship between the illumination of the photo tubes 69 and ll. As will be described, this circuit includes a pair of gaseous discharge tubes or thyratrons l2 and 13, respectively fired by the phototubes 69 and II. For extinguishing these tubes. means are provided for interrupting their anode current supply at desired intervals. As a portion of such means there is provided a pair of phototubes l5 and 16, positioned generally in a plane perpendicular to the axis of the shaft 58, but located at different angular positions with respect to said axis, as shown in Fig. 4. A lamp TI is located in a plane passing through the axis of the shaft 58, said plane approximately bi-v secting the angle subtended at said axis by the phototubes I5 and 16, as shown in Fig. i. As shown in Fig. 3, the lamp ll also lies in a plane perpendicular to the axis of the shaft 58 to the left of the phototubes l5 and 16. More particularly, the position of the lamp ll is such that a light beam from this lamp may be reflected by a light-reflecting surface 63 toward either of the phototubes 15 or 16, depending upon the angular position of the shaft. The optical path from the lamp H to the phototubes l5 and 16 is provided with collimating lenses l8, l9 and 80, as shown in Figs. 3 and 4-. As shown in Fig. 5, the thyratron 12 has a anode 85, a cathode 86, a control grid 81 and a shield grid 88. The grid 81 is controlled by the phototube 69, in a manner to be described. and the plate potential supplied to the anode 85 is controlled by the phototubes I5 and 16, in a manner which will now be described.

There is provided a thyratron which is controlled by the phototube l5 and a thyratron 90, the firing of which is controlled by asthe firing a;

the phototube 16. The firing of the thyratron 99 serves to extinguish conduction of the thyratron 89, in a manner to be described.

The general function of the various phototubes and their associated thyratrons may now be stated in a typical order of operation as the shaft rotates under a condition of torsional deflection, and subsequently a detailed explanation of the circuit will be given. It may initially be assumed that no phototubes are illuminated and that the thyratron 90 is conducting, all the other thyratrons being off.

First, the phototube I is illuminated for a short interval, firing the thyratron 89, and thereby suppling a potential to the anodes of the thyratrons l2 and 13 sufficient to support conduction. They do not, however, fire because their cathodes are held at a potential sufficiently higher than their control grids to prevent firing.

Second, the phototube H is illuminated for short interval, firing the thyratron 13.

Third, the phototube 59 is illuminated for a short interval, firing the thyratron l2 and causing conduction in the thyratron 13 to be extinguished.

Fourth, the phototube 16 is illuminated for a short interval, firing the thyratron 99, extin guishing conduction in the thyratron 89, and causing the anode supply potential to the thyratrons l2 and 13 to drop below that suificient to support conduction. Hence the thyratron I2 is extinguished.

The thyratrons are now in the condition originally assumed. It may be noted that since the grids lose control of the thyratrons after firing, the various phototubes, which control the grids, are effective in changing the condition of the circuit when the phototubes are first illuminated, and the next step in the cycle is caused not by darkening of any phototube, but by the illumination of another one.

The circuit may now be described in more detail. There is provided a source of B-supply potential such as a battery 9|, having its negative terminal grounded and its positive terminal connected to the anodes of the phototubes l5 and 16 and the thyratrons 89 and 99. The cathode 92 of the thyratron 89 is connected through a resistor 93 to a point 94, and this point is connected to ground through a resistor 95 and a parallel capacitor 95. As will appear from the subsequent description, the point 94 is normally at a positive potential with respect to ground.

The cathode 91 of the thyratronBt is connected through a resistor 98 to the point 94, and is connected through a capacitor 99 to the cathode 92 of the thyratron 89. The thyratrons 89 and are provided with anodes i911 and 1M; and with shield grids H32 and I95, respectively, connected to their cathodes.

The anode'of the phototube i5 is as stated connected to the positive terminal of the battery 9!, and the cathode is connected at a point H39 to one terminal of a resistor l 9?, the other terminal of which is grounded. Similarly the cathode of the phototube 16 is connected at a point N35 to one terminal of a resistor N9, the other terminal of which is grounded. The grid N9 of the thyratron 39 is connected through a resistor iii to the point I96, and the grid N2 of the thyratron 99 is connected through a resistor H3 to the point [98.

The cathode 92 of the thyratron 89 is connected to a point H4, which may be considered a terminal for the current supply to the plate circuits of the thyratrons I2 and 13 and the phototubes 69 and H. At the terminal H4, because of the action of the phototubes l5 and 16 and the thyratrons 89 and 90, there is available during one portion of the cycle a high positive potential, greater than suificient to support conduction in the thyratrons 12 and 13, and during another portion of the cycle only a very low positive potential, namely that appearing at the point 94, insuflicient to support conduction in the thyratrons 12 and 13.

The operation of thyratrons 89 and 90 will now be described. The characteristic of the various phototubes is that in the absence of illumination, there is negligible electron emission from their cathodes, and hence under this condition the tubes may be considered to present a high resistance at their terminals. When illuminated, there is appreciable electron emission from the cathode, and conduction may take place through the tube to an extent related to the illumination. Hence the various phototubes may be considered to present attheir terminals a low resistance when receiving considerable illumination and a high resistance when receiving little illumination. In Fig. 5, before the phototube I5 is illuminated, it represents virtually an open circuit, and hence the point I06 and the grid III) are substantially at ground potential. An initial condition may be assumed in which the thyratron 90 is conducting, having previously extinguished the thyratron 89. The plate current through the thyratron 90 flowing through the resistor to ground will elevate the potential at the point 94,

r and hence that at the cathode 92, above ground.

As a result, the grid H0 is at a potential sufficiently below that of the cathode 92 so that the tube 89 will not fire.

When the phototube 15 is illuminated, it presents a small resistance at its terminals, and because of the voltage divider action of the tube 15 in series with the resistor till, the potential at the point I 06 is elevated to such an extent that the tube 89 is fired, and the grid H9 thereafter loses control. A large plate current consequently fiows through the tube 89 and its cathode resistor 93. This current quickly elevates the potential of the cathode 92, and this rise in potential is applied through the coupling capacitor 99 to the cathode 91 of the tube 90. The capacitor 99 was previously charged because the potential at the cathode 91 was, during conduction of the tube 90, considerably above that at the point 94, while the potential at the cathode 92 was, while the tube-89 was not conducting, the same as that at the point 94. Since the voltage across a capacitor cannot instantaneously change, then it follows that when the thyratron 89 fires, the sudden rise in potential of the left-hand plate of the capacitor 99 causes the right-hand plate thereof to rise by an equal amount, and as a result, the cathode 91 of the thyratron 90 is elevated to a potential higher than the potential of the anode llll, thus extinguishing conduction of this thyratron.

When at a subsequent moment the phototube I5 is no longer illuminated and the phototube 16 is illuminated, the thyratron 99 will be caused to fire, extinguishing conduction in a similar manner in the thyratron 89.

It will therefore be understood that as the thyratron 89 is alternately turned on and oif, the potential at its cathode, and hence at the terminal H4, will rise and fall. The usefulness of such a voltage will be understood following further description of the thyratrons 12 and 13.

The thyratron 13 is provided with an anode I20, a cathode I2I, a control grid I22, and a shield grid I23. The shield grid is connected to the cathode. The anode I is connected through a resistor I24 and a resistor I25 to the terminal I I4. The junction between the resistors I24 and I25 may be indicated by the reference numeral I26. The grid I22 is connected through a grid resistor I21 to ground and is connected to the cathode of the phototube H. The anode of the phototube H, as well as the anode of the phototube 69, is connected to the terminal H t. The cathode of the phototube 69 is connected to the grid 81 of the phototube 12 and through a resistor I28 to'ground.

The cathode 86 of the thyratron 12 is connected to the point 94, and the cathode I2I of the thyratron 13 is connected through a resistor I29 to the point 94. A capacitor I30 is connected in parallel with the resistor I29. The junction of the connections to the cathode I2I, the resistor I29 and the capacitor I30 may be connected to an output terminal I3 I As will be explained, the operation of the device is such that at the terminal I3I there appears a direct current voltage proportional to or determined by the torsional deflection of the shaft. Connected between the terminal I3I and ground is a voltmeter I32, calibrated to read torque directly.

There is provided a direct current generator I33 driven by the shaft, having one terminal grounded and adapted to provide at its upper terminal I34, a positive potential proportional to the speed of rotation of the shaft. A direct current voltmeter I35 may be connected across the generator, calibrated to indicate the speed of the shaft. There is provided a multiplying device I36 responsive to the voltages at the terminals I3I and I34, adapted to produce an electrical response such as a voltage or current, proportional to the product of these voltages. In the illustrated embodiment there is shown a pentagrid converter adapted to perform this function and a direct current ammeter I31 responsive thereto. The pentagrid converter comprises a vacuum tube I38 having an anode I39, a cathode I40 and five grids, which may be designated as g1, g2, g3, g4, and g5, disposed in that order between the cathode and the anode. The anode I39 is supplied with positive potential from a terminal I4I, the instrument I31 being connected in series with the anode circuit. The

iII

cathode is connected through a resistor I42 to ground. The first control grid, grid 91, is connected to the terminal I3I. are connected together and are maintained at a relatively high positive potential by means of bleeder resistors I43 and I44, connected in series The grids g2 and g4 between the terminal I41 and the cathode I40,

the grids g2 and 9 4 being connected to the junction between the resistors I43 and I44. The bleeder resistors I43 and I44 also serve with the cathode resistor I42 to maintain the cathode at a normally positive bias potential. The grid 93, which serves as a second control grid, is connected to the terminal I34. The grid g5 is connected to the cathode I40.

The anode current through the pentagrid converter tube I38 is approximately proportional to the product of the potentials at the terminals I3I and I34, applied to the grids g1 and g3, respectively. Since these potentials are approximately proportional to the torque and speed, respectively, of the shaft, the current through the ammeter I31 is approximately proportional to trons 12 and 13.

the power transmitted by the shaft. The ammeter I31 can therefore be calibrated to read power directly.

Operation of embodiment shown in Figs. 3, 4 and 5 Let it be assumed that the thyratrons 12, 13, and 89 are in a non-conducting condition and that the thyratron is conducting. As the shaft rotates, let it now be assumed that the phototube 15 is illuminated, firing the thyratron 89 in the manner previously described, and producing at the terminal II4, a potential suflicient to initiate and support conduction in the thyra- In the absence of illumination of the phototubes 09 and H, however, these thyratrons will not fire because their grids are substantially at ground potential while their cathodes are at the potential of the point 94, which is sufiiciently above ground potential and hence above the potential of the grids, that the tubes will not fire. Very shortly after the phototube 15 is illuminated and causes appearance of a large positive potential at the terminal II4, the phototube H is illuminated because of further rotation of the shaft. Current therefore flows through the resistor I21, causing the grid I22 to assume a positive potential, and thereby firing the thyratron 13. Tortional deflection of the shaft prevents the phototube 69 from being simultaneously illuminated. It is not important whether the phototube 15 is darkened before the phototube H is illuminated or not, since the darkening of the phototube 15 does not change the potential at the point I I4. Resistors I24 and I25 in the anode circuit of the thyratron 13 are fairly large, for example, of the order of 10,000 ohms each. When only the thyratron 13 is drawing current through the resistor I25, that is, while the thyratron 12 is off, the potential at the plate I20 of the thyratron 13 is sufficient to support conduction in the thyratron 13.

As the shaft rotates still further, the phototube 69 is illuminated, causing a current to flow through the resistor I28, thereby elevating the potential of the grid 81 sufficiently to fire the phototube 12. Now that the thyratron 12 as well as the thyratron 13 is conducting, the current through the resistor I25 is of course greater than when only the thyratron 13 was conducting, and

hence the potential at the point I26 is somewhat below its previous value. The potential at this point is sufiicient, however, to support conduction in the thyratron 12. The potential at the r plate I20 of the thyratron 13, being lower than that at the point I26 by the amount of the voltage drop through the resistor I24, now falls below that necessary to sustain conduction in the thyratron 13, and this tube is extinguished. Thus when the phototube 69 is illuminated, it causes the thyratron 12 to rob the thyratron 13 of its current.

It may be seen that the duration of the interval of conduction of the thyratron 13 is determined by the lag between the time the phototube H is illuminated and the time the phototube 69 is i1- luminated which in turn is determined by the torsional deflection of the shaft.

As the shaft rotates still further the phototube 13 is illuminated, firing the thyratron 90, thereby extinguishing the thyratron 89 and causing the potential at the point I I4 to drop to such an extent that conduction in the thyratron 12 is extinguished. The thyratrons are now in the 13 same condition as that assumed at the start of the cycle.

As indicated, there flows through the thyratron I3 a series of unidirectional current pulses, each having a duration proportional to or determined by the torsional deflection of the shaft. The amplitude of the current pulses is independent of the torsional deflection. The time constant of the resistor I29 and its parallel smoothing capacitor I30 may be assumed to be large compared with the repetition period of the current pulses. Since the resistor I29 and the capacitor I30 are in series with the thyratron 73, there appears across the resistor I29 an approximately steady unidirectional voltage having a value determined by the duration of the pulses and hence by the torque transmitted by the shaft. The lower end of the resistor I29 remains at the steady potential existing at the point 94. For convenience, the voltmeter I 32, on which the torque is read, may be connected between the upper end of the resistor I29, that is, the terminal I3! and ground, and the calibration of the voltmetermay be arranged to take into account the fact that the potential of the terminal I 3| with respect to ground is slightly greater than the potential across the resistor I29, by the constant value of the potential at I the point 94.

As indicated, the torque voltage at the point I'3I and the speed voltage at the point I34 are applied to the pentagrid converter I38 which responds by producing an anode current determined by the product of these voltages, and hence determined by the power. The power may therefore be read on the ammeter I31.

Embodiment shown in Fig- 6 Reference may be made to Fig. 6 which illustrates a different embodiment of the present inventicn. It may be assumed that it is desired to measure the torque transmitted by the rotating shaft I 50 in terms of its torsional deflection. There is provided a first alternating current generator I5I driven by a first portion of the shaft, and a second alternating current generator I52, driven by a second portion of the shaft, displaced longitudinally from the first portion. The rotors of these generators may be geared to the shaft, or may be mounted on the shaft. The rotors of the respective generators are initially so aligned with respect to their stators that in the absence of torsional deflection of the shaft, the alternating voltages generated have a predetermined phase relationship. Thus, for example, they may be initially adjusted to be in quadrature, that is, out oi phase by 90 degrees. There is provided phase-sensitive comparison means, connected to the respective generators, adapted to provide a response determined by the phase difference between the voltages from the respective generators. It may be seen that this phase difference will be determined in turn by the torsional deflection of the shaft between the generators.

The phase-sensitive comparison means provided in Fig. 6 comprises a phase detector circuit, and there is provided a direct current voltmeter I53, which may conveniently be a center-scale type of instrument, connected into this phase detector circuit and responsive thereto, calibrated to read the torque transmitted by the shaft.

The generator I 5| is connected to a pair of terminals I54 and I55. The terminal I54 is connected to the terminal I55 through two parallel paths. A first or these paths comprises a resistor I56 and a resistor I51, connected: in series and having a mutual junction at a terminal I58. A

second of these paths comprises a resistor I59, a diode I, a diode I61. and a resistor I62, in series. The diode I50 is oriented so that its cathode is connected to the resistor I59 and is toward the terminal I54, while its anode is away from the terminal I54. The anode of the diode IfiI is con.- nected to. the. resistor I62 and is toward. the terminal I55, while its cathode is away from the terminal I55- The anode of the diode I50 and the cathode of the diode ISI are each connected to. a terminal I63.

One terminal of the generator I52 is connected through a large resistor I54 to the terminal I63. The other terminal of the generator I52 is connected to the terminal I58. The voltmeter I53 and an associated series resistor I53a are bridged across the terminals I53 and I 53. The illustrated resistor I531: schematically represents the internal resistance of the voltmeter and a. supplementary external resistor. Connected between the terminal I58 and a point on the resistor I53a is a capacitor I65.

Typical circuit constants are:

Resistor I56 ohms- 1000 Resistor I51 do 1000 Resistor I59 do 10,000 Resistor [52' do 10,000 Resistor I54 do 100,000 Resistor I53a (including internal resistanee of voltmeter I53) ohms 10,000 Capacitor I microfarads 4 It may be noted that the circuit constants are soproportioned that in so far as the potential applied from the generator I5I alone is concerned, the voltmeter I53 is in the position of an indi-- cating device connected into a balanced bridge. More particularly, in the particular circuit. illustrated, the resistor I 56 has the same value as. the resistor I51, namely, 1000 ohms, the resistor I59 has the same value as the resistor I62, namely, 10,000 ohms, and the diode I60 is similar to the diode I61. Thus in the two aforementioned electrical paths between the terminals I54 and I55, the terminal I58 represents the midpoint of one path, and the terminal I63 represents the midpoint in the other electrical path. In different embodiments it would not be necessary that these points represent midpoints, but it is desirable that the resistor I56 have the same ratio to the resistor I51 as does the resistor I59 to the resistor I62.

In one method of analysis of the operation of the circuit shown in Fig. 6, it is convenient to regard the alternating voltage generated by the generator I52 as the main signal to be detected, and to regard the voltage generated by the generator. I5I vas'a reference signal. It is preferable that the reference signal from the generator I5I be several times as large in amplitude as the main signal from the generator I52. Because of the aforementioned balanced relationship existing at the terminals I 58 and I 03, it may be seen that. the reference signal from the generator I5I applied to the terminals I54 and I55, cannot alone cause a deflection of the voltmeter I53.

It may be assumed that the inital adjustment of generators is such that for zero deflection either signal leads the other by degrees. As will be understood from subsequent description, zero deflection of the voltmeter results in either case.

In actual practice the torsional deflection of the shaft will always be small enough so that the resulting shift in phase of the signals from the generators is small. The shift may for example be of the order of degrees or degrees. Thus if the signals are, with no torsional deflection, out of phase by 90 degrees, they may with torsional deflection be out of phase by, for example, 80 degrees. It may be convenient, however, in analyzing the circuit to consider its operation if the torsional deflection of the shaft were such that the signals from the generators approach an in-phase condition. In the present discussion the expression in-phase may conveniently be employed to describe a condition such that terminal I54 assumes a positive potential with respect to the terminal I55 at the same time as the terminal I63 goes positive with respect to the terminal I58. It may be noted that when the terminal I54 is positive with respect to the terminal [55, the diodes I63 and I6I tend to be rendered non-conducting because of the tendency for their cathodes to be driven to a more positive potential than their anodes. Assuming an in-phase condition and assuming that the signals are in the half-cycle when the terminal I63 is positive with respect to terminal l58, it is observed that there will be in this half-cycle a flow of postive or conventional current from right to left through the voltmeter, and the right-hand plate of the capacitor !65 will become charged positively with respect to the left-hand plate. There will be no current flowing f r o m the terminal I63 to the terminal i58 via the diodes, their cathodes being at a higher potential than their anodes. In the other half-cycle, when the terminal I58 is positive with respect to the terminal I63, the terminal I55 will be positive with respect to the terminal I54, and the diodes will be rendered conducting. As a result, the effective input impedance between the terminals I58 and I63 is considerably lowered; hence the voltage drop through the large resistor I64 is sufliciently great that there is a relatively small voltage applied across the terminals I58 and I63 and hence only a small left-to-right or discharging current is supplied to the capacitor I65 by the generator I52 during this half-cycle. In view of this fact, and the additional fact that the circuit constants are so chosen that the discharge path of the capacitor through the voltmeter has a large time constant relative to the repetition period of the signals from the generator, this capacitor does not discharge appreciably during the half-cycle in question, but serves to maintain across the voltmeter a voltage of such a nature as to cause a deflection similar to that produced during the previous half-cycle.

It may therefore be seen that when the phase relationship between the signals from the generators I5I and I52 approaches an in-phase condition, positive or conventional current flows through the voltmeter I53 from right to left.

It will now be shown that, if the phase relationship between signals from the generators I5! and I52 approaches a lilo-degree out-of-phase condition, the deflection of the voltmeter I53 will be in the opposite direction. A 180-degree out of-phase condition may in the present discussion be understood to mean a phase relationship such that when the terminal I54 is positive with respect to the terminal (55, the terminal IE3 is negative with respect to the terminal I53. With such a phase relationship and in the half-cycle when the last-mentioned conditions exist, the (iiodes will be non-conducting and there will be a' flow of current from the terminal I58 through the voltmeter from left to right toward the terminal I 63, with a consequent charging of the condenser I65 so that its left-hand plate is positive with respect to its right-hand plate. During the other half-cycle, the diodes will be rendered conducting because of the fact that the terminal I55 is positive with respect to the terminal I54. As a result, there will exist between the terminals I58 and I33 a current path through the diodes as well as through the voltmeter. A larger current consequently flows through the resistor I64 producing such a voltage drop therein that only a small voltage is impressed across the terminals I63 and I58, and the capacitor I65 is not discharged to any great extent but is capable of maintaining a flow of current through the voltmeter from left to right, so as to maintain the deflection in the same direction as during the previous half-cycle. It may therefore be seen thatif the signals from the generators I5I and I52 approach a 180-degree out-of-phase condition the deflection of the voltmeter is in a direction opposite to its direction of deflection when the signals are in phase.

Analysis will show that if the signals are in quadrature, that is, degrees out-of-phase, the capacitor I65 will be partially charged first in one direction and then in the other, and there will result a net zero deflection of the voltmeter, particularly in view of the fact that its moving elements have a certain amount of inertia.

In actual operation, the system of Fig. 6 may be, as stated, initially adjusted so that when there is no torsional deflection of the shaft, the signals from the generators I 5I and I52 are in quadrature, and there is zero deflection of the voltmeter. When there is torsional deflection of the shaft, the voltmeter will be deflected to an extent dependent upon the amount of torsional deflection of the shaft, and approximately linearly therewith for small angles of torsional deflection. The voltmeter 153 may therefore be calibrated to read torque directly. It will be noted that the direction of deflection of the voltmeter will indicate the direction of the torsional deflection.

It may be assumed that the alternatingcurrent generators I5I and I52 include means not shown in detail for producing magnetic fields, and movable windings adapted to interrupt or cut through said fields for generating alternating voltages or for producing modulation effects. Hence in Fig. 6 there is provided a first movable element driven through a magnetic field by a first portion of the shaft, a second movable element driven through a magnetic field by a second portion of the shaft displaced longitudinally from the first portion, the respective motions of the movable elements having a phase difference determined by the torsional deflection of the shaft between these longitudinally spaced portions, and comparison means responsive to this phase difference adapted to produce a measurement dependent upon the said deflection.

Embodiment shown in Fig. 7

Reference is made to Fig. '1 which illustrates a different embodiment of the invention. It may be assumed that it is desired to measure the torsional deflection of a rotating shaft I10. There are provided a plurality of control transformers of the synchro types "I and I12 having rotors and stators. The rotor I13 of the synchro III is driven by a first portion of the shaft I10. This rotor may be mounted directly on the shaft or may be driven by suitable gears as illustrated,

Thus the shaft I10 may carry a gear I14 which drives a gear I15. The gear I15 may be mounted on a shaft I18, which in turn carries the rotor I13. The rotor I18 of the synchro I12 is similarly driven by a portion of the shaft I10 displaced longitudinally thereof from the portion which drives the rotor I13. Thus the shaft I10 may carry a gear I19 which drives a gear I80, which in turn drives a shaft I8I on-which the rotor I18 is mounted. The ratios of the respective systems of gears should be the same, and mayconveniently be arranged so that a small torsional deflection of the shaft produces a somewhat larger relative torsional deflection between the rotors.

The rotor I13 of the synchro I1I may comprise a single winding energized by a source I82 of alternating voltage. The stators of the synchros may comprise delta or Y-type windings, connected in parallel. The stator of the synchro "I may be designated by the numeral I83 and that of the synchro I12 by the numeral I84. i

It will be understood that as the energized winding I13 is rotated, it produces a rotating alternating magnetic field in its vicinity, thereby inducing currents in the stator I83 of the synchro I1 I. Since the two stators are connected in parallel, similar currents are caused to flow in the stator I84 of the synchro I12, and a similar rotating alternating magnetic field is produced the synchro I12. Therotor I18 of the synchro I12 may comprise a-single winding having output terminals I85 and I86. The system may initially be aligned so that when there is no torsional deflection of the shaft the rotor windings I13 and I18 are positioned in quadrature arrangement.

That is, the rotating magnetic field produced in the region of the rotor I18 is oriented relative to this rotor so that substantially none of it links the winding I18, and hence zero voltage is induced in this winding. Thus the rotor I18 is rotated at the same speed as the magnetic field in the region thereof, but it is so positioned with respect to this field that there is, as stated, no voltage induced in the rotor I18. 1

When there is torsional deflection of the shaft, the position of the rotor I18 relative to the magnetic field in the region thereof will be changed so that there is a voltage induced in this rotor. As a result there appears across the terminals I85 and I86, an alternating voltage determined by the torsional deflection of the shaft and proportional thereto for small angles of deflection. A voltmeter I81 may be connected across these terminals and may be calibrated to indicate torque directly.

The rotor I13 may be viewed as a primary winding, and the stator I83 may be considered to comprise a secondary winding of the synchro I1I since the winding I13 induces currents in the winding I583. In the synchro I12, the stator I84 may be considered to comprise a primary winding, and the rotor I18 may be considered to comprise a secondary winding since the winding I18 is en-- ergized only as a result of currents flowing in the winding I84.

It may be observed that, in a sense, the rotation of the rotor I18 serves to counteract the voltageproducing efiect of the rotation of the rotor I13 to a degree related to the torsional deflection of the shaft. That is, if the rotor I18 were not rotated, the rotation of the rotor I13 would produce a considerable voltage effect at the voltmeter I81, but rotation of the rotor I18 at the same speed as the magnetic field in the region thereof serves in a sense to counteract this voltage-producing effect. The counteraction is complete if there is no torsional deflection of the shaft in view of the original quadrature arrangement of the rotors, and is lesscompl'ete if there is such a torsional deflection.

The system'of Fig. 7 is adapted for indicating power as. well as torque. In case it is desired to measure power, there may be provided a generatorv I88 having a rotor I89 and a stator or field winding- I90." The rotor I89 is driven at a speed proportional to the speed of the shaft I 10, and may for example be carried by the shaft I8 I. The winding I90 is in the present embodiment supplied with a direct current proportional to or dependent upon the torque of the shaft I10. For this purpose there is provided rectifying means, and the terminals I and I88 are connected through said rectifying means to the winding I90. Comprising the aforementioned rectifying means, there is provided a diode HI and a resistor I 92 connected in series across the terminals I85 and I88. The voltage appearing across the resistor I 92 is filtered, as by a lI-type filter comprising a series inductor I 93 and shunt capacitors I94 and I95. The direct current from this filter which is applied to the winding I90, is approximately proportional to the torque transmitted by the shaft I18.

The winding I will induce in the region of the rotor I89 a unidirectional magnetic field determined by the torque transmitted by the shaft. The rotor I89 will be rotated at a speed determined by the speed of the shaft, and as a consequence there will be induced in the winding of the rotor I89 an alternating voltage determined by the product of the speed and the torque of the shaft, and hence determined by the power transmitted by the shaft. An alternating current voltmeter I96 calibrated to read power directly, may be connected across the winding of the rotor I89.

While the generator I 88 in Fig. '1 has been shown as an alternator, it is possible to utilize a direct current generator and a direct current voltmeter, if desired.

As a variation, in case it is desired to secure a large output voltage, an amplidyne may be substituted in place of the generator I88.

In summary, it may be seen that there has been described an accurate and inexpensive apparatus and method for measuring the torque or the power transmitted by the rotating shaft. Thus there is provided, in combination, means comprising elements driven by longitudinally spaced portions of the shaft for producing energy variations dependent upon the torsional deflection between said shaft portions and measuring means controlled by said energy variations.

In certain embodiments there are provided means for producing a field of light, and in other embodiments there are provided means for producing a magnetic field. There are provided field-interrupting means, and means driven by longitudinally spaced portions of the shaft for causing relative motion between said field-interrupting means and the field itself, and for thereby causing modulation effects dependent upon the torsional deflection of the shaft. The modulation effects in turn may be employed to produce an indication of the torque. In case it is desired to measure power, the modulation effects may be employed to produce an electrical response proportional to torque, and this re 19' spouse, togetherwith a response proportional to the speed of the shaft, maybe applied to a multiplying device adapted' to produce an indication of the power transmitted by the shaft.

While a suitable form of apparatus and mode of procedure to be used in accordance with the invention have been described in some detail, and certain modifications have been suggested, it will be understood that numerous changes may be madewithout departing from the general principles' and scope of the invention.

What is claimed is:

1. In apparatus for measuring the torsional defiection of a rotating shaft, first and second separate light modulators, said first modulator including a first movable member; said second light modulator including. a second movable member, said members being respectively driven by two longitudinally spaced portions of said shaft, each of said members comprising alternate light-reflecting and light-absorbing surface areas, a light beamdirected toward each of said members, a first phototubefor said first light modulator, a second phototube for said second light modulator, said light modulatorsbeing adapted to transmit to said phototubes modulated light beams difiering in phase by an amount determined by the relative torsional deflection between said spaced portions of said shaft, said members being oriented with relation to one another in such manner that when there is no torsional deflection said first and second phototubes are simultaneously illuminated and simultaneously darkened, and when there is torsional deflection said first phototube illuminated before said second phototube, a phase-sensitive comparison circuit connected to said first and second phototubes for producing a series of unidirectional current pulses each having a duration determined by the torsional deflection of said shaft, said circuit comprising first and second thyratrons respectively fired by said first and second phototubes, said first thyratron' comprising an anode and a cathode, said second thyratron comprising an anode, a source of anode current supply, a terminal connected to said anode current supply, each of said anodes connected to said terminal, means for interrupting said anode current supply at intervals corresponding to the number of lightrefiecting surface areas on said-- first movable member, said means comprising thirdand fourth phototubes positioned in a plane perpendicular to the axis of said first movable member, said I phototubes being located at difierent angular positions with respect to the axis of said member, a light beam located in aplane passing through the axis of said member in such manner as to bisect the angle subtended at said axis by said or said member toward said third phototube-and then toward said fourth phototubein accordance withithe angular position of said'rotatingsh'aft, a third thyratron connected to" said third phototube and adapted to befired thereby prior to the firing of saidlfirst and second thyratrons, said" third thyratron being connected to said anode current supply source and to said anode current supply terminal and being adapted while conducting to supply a potential to said anode current supply terminal sufiicient to support the conduction of said first and second thyratrons, a fourth thyratron connected tosaid fourth phototube and adapted to be firedthereby subsequent to the firing.- of said first and secondthyratrons, said fourth thyratron being connected to said third thyratron and adapted on being fired to extinguish the conduction of said third thyratron, circuit means connected between said anode current supplyterminal and the anodes of said first-and second thyratrons for lowering the anode potential ofsaid first thyratron below the value required to support conduction of said first thyratron on firing said second thyratron and thereby producing through said first thyratron said-series of unidirectional current pulses, circuit means connected to the cathode of said first thyratron for providing a steady unidirectionalvoltage having: a'valuedetermined by the duration of said unidirectional current pulses and hence by the torque transmitted by said shaft.

2. Apparatus in accordance with claim 1 ineluding. a generator driven by said shaft and adaptedto produce a voltage-proportional to the speed of rotation of said shaft, a multiplying device responsive to the voltage produced by said generatorand to said unidirectional voltage determined by the torque transmitted by said shaft and adapted to produce an electrical response proportional to the product o'fsaid voltages, and an indicating instrument responsive to said multiplying device adapted to indicate the power transmitted by said shaft.

REFERENCES" CITED The following references are of record in the file of thispatent:

UNITED STA DES PATENTS Number Name Date T585364 Smith et al; Oct. 2, 1928 1,721,375 Koning July 16', 1929 2,077,220" Smith July 9, 1935 2,0501866' Tamm' Aug. 11, 1936 2,136,223 Thomas Nov. 8, 1938 2,176,935 Smith Oct. 24, I939 231531923 Chubb' Mar. 16, 1943 2346;976 Banger et al; Apr. 1-8, 1944 2,40'2fil9 Allison June 25, 1946 

